Light Z′ and Dirac fermion dark matter in the B-L model
We consider a U ( 1 ) B - L model with a Z ′ portal Dirac fermion dark matter (DM) χ of low mass which couples very weakly to the B - L gauge boson Z ′ . An arbitrary B - L charge Q ≠ ± 1 , ± 3 of the DM χ ensures its stability. Motivated by the sensitivity reach of forthcoming “Lifetime Frontier” e...
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Veröffentlicht in: | The European physical journal. C, Particles and fields Particles and fields, 2022-10, Vol.82 (10) |
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Hauptverfasser: | , , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
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Zusammenfassung: | We consider a
U
(
1
)
B
-
L
model with a
Z
′
portal Dirac fermion dark matter (DM)
χ
of low mass which couples very weakly to the
B
-
L
gauge boson
Z
′
. An arbitrary
B
-
L
charge
Q
≠
±
1
,
±
3
of the DM
χ
ensures its stability. Motivated by the sensitivity reach of forthcoming “Lifetime Frontier” experiments, we focus on the
Z
′
mass,
m
Z
′
, in the sub-GeV to few GeV range. To evaluate the DM relic abundance, we examine both the
freeze-out
and
freeze-in
DM scenarios. For the
freeze-out
scenario, we show that the observed DM abundance is reproduced near the
Z
′
resonance,
m
χ
≃
m
Z
′
/
2
, where
m
χ
is the DM mass. For the
freeze-in
scenario, we focus on
m
χ
≪
m
Z
′
. We show that for a fixed value of
m
Z
′
,
g
BL
values roughly scale as 1/
Q
to reproduce the observed DM abundance. For various
Q
values in the range between
10
-
6
and
10
2
, we show that the gauge coupling values
g
BL
needed to reproduce the observed DM abundance lie in the search reach of future planned and/or proposed experiments such as FASER, Belle-II, LDMX, and SHiP. In the
freeze-in
case, the
Q
values to realize observable
g
BL
values are found to be much smaller than that in the
freeze-out
case. |
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ISSN: | 1434-6044 1434-6052 |
DOI: | 10.1140/epjc/s10052-022-10801-3 |